Stephen M. Griffies, Alistair Adcroft, Rebecca L. Beadling, Mitchell Bushuk, Chiung-Yin Chang, Henri F. Drake, Raphael Dussin, Robert W. Hallberg, William J. Hurlin, Hemant Khatri, John P. Krasting, Matthew Lobo, Graeme A. MacGilchrist, Brandon G. Reichl, Aakash Sane, Olga Sergienko, Maike Sonnewald, Jacob M. Steinberg, Jan-Erik Tesdal, Matthew Thomas, Katherine E. Turner, Marshall L. Ward, Michael Winton, Niki Zadeh, Laure Zanna, Rong Zhang, Wenda Zhang, Ming Zhao
{"title":"GFDL-CM4X气候模式层次,第一部分:模式描述和热性质","authors":"Stephen M. Griffies, Alistair Adcroft, Rebecca L. Beadling, Mitchell Bushuk, Chiung-Yin Chang, Henri F. Drake, Raphael Dussin, Robert W. Hallberg, William J. Hurlin, Hemant Khatri, John P. Krasting, Matthew Lobo, Graeme A. MacGilchrist, Brandon G. Reichl, Aakash Sane, Olga Sergienko, Maike Sonnewald, Jacob M. Steinberg, Jan-Erik Tesdal, Matthew Thomas, Katherine E. Turner, Marshall L. Ward, Michael Winton, Niki Zadeh, Laure Zanna, Rong Zhang, Wenda Zhang, Ming Zhao","doi":"10.1029/2024MS004861","DOIUrl":null,"url":null,"abstract":"<p>We present the GFDL-CM4X (Geophysical Fluid Dynamics Laboratory Climate Model version 4X) coupled climate model hierarchy. The primary application for CM4X is to investigate ocean and sea ice physics as part of a realistic coupled Earth climate model. CM4X utilizes an updated MOM6 (Modular Ocean Model version 6) ocean physics package relative to CM4.0, and there are two members of the hierarchy: one that uses a horizontal grid spacing of <span></span><math>\n <semantics>\n <mrow>\n <mn>0.25</mn>\n <mo>°</mo>\n </mrow>\n <annotation> $0.25{}^{\\circ}$</annotation>\n </semantics></math> (referred to as CM4X-p25) and the other that uses a <span></span><math>\n <semantics>\n <mrow>\n <mn>0.125</mn>\n <mo>°</mo>\n </mrow>\n <annotation> $0.125{}^{\\circ}$</annotation>\n </semantics></math> grid (CM4X-p125). CM4X also refines its atmospheric grid from the nominally 100 km (cubed sphere C96) of CM4.0–50 km (C192). Finally, CM4X simplifies the land model to allow for a more focused study of the role of ocean changes to global mean climate. CM4X-p125 reaches a global ocean area mean heat flux imbalance of <span></span><math>\n <semantics>\n <mrow>\n <mo>−</mo>\n <mn>0.02</mn>\n <mspace></mspace>\n <mi>W</mi>\n <mspace></mspace>\n <msup>\n <mi>m</mi>\n <mrow>\n <mo>−</mo>\n <mn>2</mn>\n </mrow>\n </msup>\n </mrow>\n <annotation> ${-}0.02\\hspace*{.5em}\\mathrm{W}\\hspace*{.5em}{\\mathrm{m}}^{-2}$</annotation>\n </semantics></math> within <span></span><math>\n <semantics>\n <mrow>\n <mi>O</mi>\n <mrow>\n <mo>(</mo>\n <mn>150</mn>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation> $\\mathcal{O}(150)$</annotation>\n </semantics></math> years in a pre-industrial simulation, and retains that thermally equilibrated state over the subsequent centuries. This 1850 thermal equilibrium is characterized by roughly <span></span><math>\n <semantics>\n <mrow>\n <mn>400</mn>\n <mspace></mspace>\n <mtext>ZJ</mtext>\n </mrow>\n <annotation> $400\\hspace*{.5em}\\text{ZJ}$</annotation>\n </semantics></math> less ocean heat than present-day, which corresponds to estimates for anthropogenic ocean heat uptake between 1870 and present-day. CM4X-p25 approaches its thermal equilibrium only after more than 1000 years, at which time its ocean has roughly <span></span><math>\n <semantics>\n <mrow>\n <mn>1100</mn>\n <mspace></mspace>\n <mtext>ZJ</mtext>\n </mrow>\n <annotation> $1100\\hspace*{.5em}\\text{ZJ}$</annotation>\n </semantics></math> <i>more</i> heat than its early 21st century ocean initial state. Furthermore, the root-mean-square sea surface temperature bias for historical simulations is roughly 20% smaller in CM4X-p125 relative to CM4X-p25 (and CM4.0). We offer the <i>mesoscale dominance hypothesis</i> for why CM4X-p125 shows such favorable thermal equilibration properties.</p>","PeriodicalId":14881,"journal":{"name":"Journal of Advances in Modeling Earth Systems","volume":"17 10","pages":""},"PeriodicalIF":4.6000,"publicationDate":"2025-10-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://agupubs.onlinelibrary.wiley.com/doi/epdf/10.1029/2024MS004861","citationCount":"0","resultStr":"{\"title\":\"The GFDL-CM4X Climate Model Hierarchy, Part I: Model Description and Thermal Properties\",\"authors\":\"Stephen M. Griffies, Alistair Adcroft, Rebecca L. Beadling, Mitchell Bushuk, Chiung-Yin Chang, Henri F. Drake, Raphael Dussin, Robert W. Hallberg, William J. Hurlin, Hemant Khatri, John P. Krasting, Matthew Lobo, Graeme A. MacGilchrist, Brandon G. Reichl, Aakash Sane, Olga Sergienko, Maike Sonnewald, Jacob M. Steinberg, Jan-Erik Tesdal, Matthew Thomas, Katherine E. Turner, Marshall L. Ward, Michael Winton, Niki Zadeh, Laure Zanna, Rong Zhang, Wenda Zhang, Ming Zhao\",\"doi\":\"10.1029/2024MS004861\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>We present the GFDL-CM4X (Geophysical Fluid Dynamics Laboratory Climate Model version 4X) coupled climate model hierarchy. The primary application for CM4X is to investigate ocean and sea ice physics as part of a realistic coupled Earth climate model. CM4X utilizes an updated MOM6 (Modular Ocean Model version 6) ocean physics package relative to CM4.0, and there are two members of the hierarchy: one that uses a horizontal grid spacing of <span></span><math>\\n <semantics>\\n <mrow>\\n <mn>0.25</mn>\\n <mo>°</mo>\\n </mrow>\\n <annotation> $0.25{}^{\\\\circ}$</annotation>\\n </semantics></math> (referred to as CM4X-p25) and the other that uses a <span></span><math>\\n <semantics>\\n <mrow>\\n <mn>0.125</mn>\\n <mo>°</mo>\\n </mrow>\\n <annotation> $0.125{}^{\\\\circ}$</annotation>\\n </semantics></math> grid (CM4X-p125). CM4X also refines its atmospheric grid from the nominally 100 km (cubed sphere C96) of CM4.0–50 km (C192). Finally, CM4X simplifies the land model to allow for a more focused study of the role of ocean changes to global mean climate. CM4X-p125 reaches a global ocean area mean heat flux imbalance of <span></span><math>\\n <semantics>\\n <mrow>\\n <mo>−</mo>\\n <mn>0.02</mn>\\n <mspace></mspace>\\n <mi>W</mi>\\n <mspace></mspace>\\n <msup>\\n <mi>m</mi>\\n <mrow>\\n <mo>−</mo>\\n <mn>2</mn>\\n </mrow>\\n </msup>\\n </mrow>\\n <annotation> ${-}0.02\\\\hspace*{.5em}\\\\mathrm{W}\\\\hspace*{.5em}{\\\\mathrm{m}}^{-2}$</annotation>\\n </semantics></math> within <span></span><math>\\n <semantics>\\n <mrow>\\n <mi>O</mi>\\n <mrow>\\n <mo>(</mo>\\n <mn>150</mn>\\n <mo>)</mo>\\n </mrow>\\n </mrow>\\n <annotation> $\\\\mathcal{O}(150)$</annotation>\\n </semantics></math> years in a pre-industrial simulation, and retains that thermally equilibrated state over the subsequent centuries. This 1850 thermal equilibrium is characterized by roughly <span></span><math>\\n <semantics>\\n <mrow>\\n <mn>400</mn>\\n <mspace></mspace>\\n <mtext>ZJ</mtext>\\n </mrow>\\n <annotation> $400\\\\hspace*{.5em}\\\\text{ZJ}$</annotation>\\n </semantics></math> less ocean heat than present-day, which corresponds to estimates for anthropogenic ocean heat uptake between 1870 and present-day. CM4X-p25 approaches its thermal equilibrium only after more than 1000 years, at which time its ocean has roughly <span></span><math>\\n <semantics>\\n <mrow>\\n <mn>1100</mn>\\n <mspace></mspace>\\n <mtext>ZJ</mtext>\\n </mrow>\\n <annotation> $1100\\\\hspace*{.5em}\\\\text{ZJ}$</annotation>\\n </semantics></math> <i>more</i> heat than its early 21st century ocean initial state. Furthermore, the root-mean-square sea surface temperature bias for historical simulations is roughly 20% smaller in CM4X-p125 relative to CM4X-p25 (and CM4.0). We offer the <i>mesoscale dominance hypothesis</i> for why CM4X-p125 shows such favorable thermal equilibration properties.</p>\",\"PeriodicalId\":14881,\"journal\":{\"name\":\"Journal of Advances in Modeling Earth Systems\",\"volume\":\"17 10\",\"pages\":\"\"},\"PeriodicalIF\":4.6000,\"publicationDate\":\"2025-10-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://agupubs.onlinelibrary.wiley.com/doi/epdf/10.1029/2024MS004861\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Advances in Modeling Earth Systems\",\"FirstCategoryId\":\"89\",\"ListUrlMain\":\"https://agupubs.onlinelibrary.wiley.com/doi/10.1029/2024MS004861\",\"RegionNum\":2,\"RegionCategory\":\"地球科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"METEOROLOGY & ATMOSPHERIC SCIENCES\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Advances in Modeling Earth Systems","FirstCategoryId":"89","ListUrlMain":"https://agupubs.onlinelibrary.wiley.com/doi/10.1029/2024MS004861","RegionNum":2,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"METEOROLOGY & ATMOSPHERIC SCIENCES","Score":null,"Total":0}
The GFDL-CM4X Climate Model Hierarchy, Part I: Model Description and Thermal Properties
We present the GFDL-CM4X (Geophysical Fluid Dynamics Laboratory Climate Model version 4X) coupled climate model hierarchy. The primary application for CM4X is to investigate ocean and sea ice physics as part of a realistic coupled Earth climate model. CM4X utilizes an updated MOM6 (Modular Ocean Model version 6) ocean physics package relative to CM4.0, and there are two members of the hierarchy: one that uses a horizontal grid spacing of (referred to as CM4X-p25) and the other that uses a grid (CM4X-p125). CM4X also refines its atmospheric grid from the nominally 100 km (cubed sphere C96) of CM4.0–50 km (C192). Finally, CM4X simplifies the land model to allow for a more focused study of the role of ocean changes to global mean climate. CM4X-p125 reaches a global ocean area mean heat flux imbalance of within years in a pre-industrial simulation, and retains that thermally equilibrated state over the subsequent centuries. This 1850 thermal equilibrium is characterized by roughly less ocean heat than present-day, which corresponds to estimates for anthropogenic ocean heat uptake between 1870 and present-day. CM4X-p25 approaches its thermal equilibrium only after more than 1000 years, at which time its ocean has roughly more heat than its early 21st century ocean initial state. Furthermore, the root-mean-square sea surface temperature bias for historical simulations is roughly 20% smaller in CM4X-p125 relative to CM4X-p25 (and CM4.0). We offer the mesoscale dominance hypothesis for why CM4X-p125 shows such favorable thermal equilibration properties.
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